U. Behrens et al., STRUCTURE, DIELECTRIC-RELAXATION AND ELECTRICAL-CONDUCTIVITY OF ANTHRENE-2,3-DICHLORO-5,6-DICYANO-1,4-BENZOQUINONE 1 1 CHARGE-TRANSFER COMPLEXES/, Journal of materials chemistry, 6(4), 1996, pp. 547-553
2,3,7,8-Tetramethoxychalcogenanthrenes (5,10-chalcogena-cyclo-diveratr
ylenes, 'Vn(2)E(2)', E = S, Se) form isotypical 1:1 charge-transfer (C
T) complexes with 2,3-dichloro-5,6-dicyano-1,4-benzoquinone (DDQ). X-r
ay analysis of Vn(2)S(2) . DDQ shows the compound to have a columnar s
tructure with segregated stacks of donors and acceptors. The donors ar
e virtually planar in accordance with a formulation of [Vn(2)E(2)](+)[
DDQ](-). Donor cations and acceptor anions are equidistant in their re
spective stacks, but in each case they inclined to the stacking axis,
nevertheless guaranteeing an optimum overlap of the half-filled fronti
er orbitals which are of pi-type character according to MNDO calculati
ons. Dielectric ac measurements of permittivity epsilon' and loss fact
or E '' clearly reveal two processes, a dielectric one at low temperat
ures and a conductive one at high temperatures. The dielectric process
can be described by the Havriliak-Negami (HN) and the Kohlrausch-Will
iams-Watts (KWW) model, and the conductive process by a Debye-type plo
t. Using these methods, the relevant parameters are evaluated. The de
conductivities of polycrystalline samples moulded at 10(8) Pa show a t
emperature dependence in the plots of ln sigma vs. T-1, which is typic
al of semiconductors. Two slopes are found; that in the low-temperatur
e region (<285 K) is explained by an easy-path model (intragrain condu
ctivity with low activation energies), whereas in the high-temperature
region conduction across the grain boundaries (with higher activation
energies) is becoming predominant. The activation energies for the in
trinsic conductivities obtained by the ac and de measurements are simi
lar. Despite the columnar structure with segregated stacks, due to sto
ichiometric oxidation states of the components, the absolute values of
conductivity are low ten. 10(-6) S cm(-1) at 293 K), though higher (b
y a factor of ca. 10(3)) than those of compounds like Vn(2)E(2) . TCNQ
with stacks in which donor and acceptor molecules alternate.